Diagram showing Martin’s M-275 supersonic seaplane bomber design from a NACA report.
Introduction The previous volume described the development of American supersonic bombers that got as far as obtaining an official designation from the Department of Defense. But that is hardly a comprehensive list of all American supersonic bombers; a vast number of them have been designed but got no further than proposals. Some, not even that far. A lack of development does not, however, denote a lack of interest. This volume will describe a wide range of designs that have been put forward over the course of around three quarters of a century. As with the first volume, the definition of a ‘bomber’ is a little vague… an aircraft designed from
the outset to carry bombs (or missiles meant to strike ground targets). With one rather outstanding exception, the bomber is intended for recovery and re-use. Given the vast number of supersonic bombers designed, organising them in a sensible manner that everyone can agree on would be virtually impossible. So here the author has chosen a reasonable number and organised them into a few distinct groups: seaplanes, nuclear powered, nuclear powered seaplanes, vertical takeoff and landing, hypersonic.
Scott Lowther
aerospaceprojectsreview.com Author/artist: Scott Lowther Publisher: Steve O’Hara Published by: Mortons Media Group Ltd, Media Centre, Morton Way, Horncastle, Lincolnshire LN9 6JR, Tel. 01507 529529
Contents Chapter 1: N uclear Powered Supersonic Bombers
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Chapter 2: Seaplanes
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Chapter 3: N uclear Powered Seaplane Supersonic Bombers 69 Chapter 4: VTOL Bombers
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Chapter 5: Hypersonics
107
References
128
General data table
129
Typeset by: Druck Media Pvt. Ltd. Printed by: Acorn Web Offset Ltd, Loscoe Close, Normanton Industrial Estate, West Yorkshire WF6 1TW All diagrams ©2023 Scott Lowther Acknowledgements: This book could not have been completed without the assistance of a number of authors and historians, including but not limited to: Dennis Jenkins, Tony Landis, Tony Buttler. Their assistance and contributions are greatly appreciated. ISBN: 978-1-911703-18-1 © 2023 Mortons Media Group Ltd. All rights reserved. No part of this publication may be reproduced or transmitted in any form or by any means, electronic or mechanical, including photocopying, recording, or any information storage retrieval system without prior permission in writing from the publisher.
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CHAPTER
B
Nuclear Powered Supersonic Bombers
y the end of the Second World War the United States was on the verge of fielding bombers that could reach European targets from American bases and return, all on a single load of fuel. Aircraft such as the Convair B-36 had incredible ranges, but the requirements turned the aircraft into flying fuel tanks. The advent of jet engines made the range problem even worse: the new engines could raise top speed, but at the expense of even greater fuel consumption. The use of turboprops would theoretically improve on the maximum airspeed of piston engined aircraft, while increasing the range over that of pure turbojet designs; even so, the improvements were not spectacular. There were few options for improved fuels, though some hope was held out for propellants such as liquid hydrogen. In the end, the Strategic Air Command was able to raise the range of bombers to truly global, with mission durations measured potentially in days through the use of in-flight refuelling. This has worked well over the decades, but it ties the bomber to slow and vulnerable tanker aircraft. Another option was studied shortly after the end of the Second World War. Immediately following the detonations of Little Boy and Fat Man the world entered the Atomic Age and for a while it seemed that the friendly atom could do just about anything. It proved that it could cleanly light cities and run factories; it also proved practical to power submarines and aircraft carriers. There were proposals to use nuclear power to create instant ports and sea-level canals across Nicaragua and to send giant space vehicles to Mars and beyond. And it was studied in some considerable depth as a means of powering aircraft. The basic notion of atomic energy to power aircraft existed in both the United States and Germany during the Second World War, but it seems it was little more than that: notional. Practical reactor engineering design was as yet unknown in the United States, and virtually impossible in Nazi Germany. Nevertheless, things were moving quickly. In May 1946, the United States Army Air Force awarded a contract to Fairchild Engine and Aircraft Corporation to begin the study of Nuclear Energy for the Propulsion of Aircraft (NEPA). NEPA was instituted to both perform basic feasibility studies and to provide information to the American aircraft engine 4
industry on nuclear issues. At first highly hypothetical, NEPA and its successor programmes would go on to build nuclear powered jet engines and create detailed designs of atomic-powered aircraft. However, in the early years the programme was populated by experts who felt that atomic-powered aircraft were only a few hard-working years away, and others who felt that the whole concept bordered on the ludicrous. In 1948, the Massachusetts Institute of Technology was brought on board in large part to finally settle the matter. MIT scientists concluded that nuclear flight was possible, though they estimated that it would take 15 years and a billion dollars to achieve. This was when even the United States government felt that a billion dollars was a fairly large sum of money. Two main engine types were looked at under NEPA. The ‘Direct Cycle’ ducts air from an inlet directly into the reactor. Air flows through the reactor itself, coming in physical contact with reactor fuel elements. The reactor running at high power generates a vast amount of heat energy; left alone, the reactor would melt. But the air flowing through the Direct Cycle reactor cools the fuel, preventing damage to the hot structure. In the process, the air becomes superheated. This hot blowtorch of air is ejected aft at high speed, generating thrust directly, or flows through a series of turbines, providing the power needed to turn either propellers or a compressor stage. The Direct Cycle engine is simple and effective and quite efficient; but white-hot oxygen and nitrogen – not to mentions bugs and dust – will do the uranium fuel elements no good whatsoever. A Direct Cycle engine stands a very good chance of ejecting a constant spray of tiny bits of the engine, leaving a radioactive trail wherever the aircraft may go. This is generally considered undesirable, especially when flying over friendly territory. The Indirect Cycle engine avoids the environmental hazards – as well as extending the life of the reactor – by inserting a heat exchanger between the fuel and the air. The reactor is cooled not by air flowing through it at high pressure and velocity, but by something like liquid sodium metal. The superheated molten metal then flows through a heat exchanger, transferring its energy to air. The heat exchanger is generally located in the part of a turbojet or turboshaft engine normally occupied by the combustors, replacing the chemical fuels contribution to the engine cycle.
Nuclear Powered Supersonic Bombers
The Indirect method is heavier and more complex than Direct, but it has many obvious advantages. Not least of these is that since the liquid metal is very dense compared to air, it can be piped elsewhere, to heat exchangers located far from the reactor. Thus where Indirect systems generally required that the reactors and the jet engine be either integrated units or at least located very close to each other, the Indirect system allows for reactors to be deeply buried in the fuselage while the jet engines can be located far out along the wings. In addition, while the Indirect system introduces inefficiencies due to the added steps, the fact is that a liquid metal, being many times denser than compressed air, is far more effective at removing heat from the reactor. In addition, a liquid metal is unlikely to chemically interact with the reactor, while whitehot oxygen is quite effective at oxidizing virtually anything. These two methods allowed for a wide range of possible engine and aircraft configurations. But one thing that remained consistent was that nuclear propulsion for aircraft was monstrously heavy. The reactor was, compared to the chemical fuel, generally relatively light, but the plastic and lead radiation shielding, typically surrounding the reactor and again surrounding the crew, located as far as engineeringly possible from the reactor, were massive. And as powerful as an atomic reactor may sound, in practice they often struggled to produce power outputs equal to those of conventional turbojet engines at full thrust. The result was that the vast majority of the designs for atomic powered aircraft were strictly subsonic. Even then they often required chemical fuel augmentation for takeoff. Nevertheless, the occasional nuclear powered design was produced that was capable of exceeding Mach One. The designs were often unconventional to say the least. A note on shielding: most designs included shielding around the reactor, and further shielding around the cockpit. Generally the shielding was a mix of heavy metal such as lead or tungsten and a light plastic like polyurethane or rubber, often with additional water tanks (sometimes with boron compounds dissolved or mixed in as well). This composite was due to the fact that dense metals are effective at shielding against gamma rays, while plastics contain a fair amount of hydrogen which absorbs neutrons. In general the cockpit was placed as far as possible from the reactor, with as much of the aircraft structure as possible between the two to serve as further shielding. At first glance it may seem that it would only be necessary to place radiation shields directly between the reactor and the cockpit, but the shielding generally fully encompassed the cockpit on all sides including the
front. This is because the radiation would be scattered by the air surrounding the craft. A way to think of it is that the reactor was an intensely bright light bulb, and the air surrounding the cockpit was filled with fog: the light bulb may have been well behind the cockpit, but light would still come pouring in from the front due to being reflected by the fog. The radiation would be reflected by the air molecules in the same fashion and would quickly irradiate the crew if they were not shielded on all sides. This included the windows: they would need to be made of thick leaded glass and Plexiglas in order to absorb the incoming radiation. Further, radiation would be reflected from the metallic structure of the aircraft including wings and the fuselage; anything that could be seen from the cockpit would be a source of incoming radiation. So while some designs featured expansive cockpit canopies, in general those were only the transparent aerodynamic fairings that covered the real windows… thick, small transparencies that protected the crew. One of the advantages of a nuclear propulsion system for aircraft is also a problem for the aircraft. An aircraft that burns a large amount of fuel weighs considerably less at the end of its flight than it did at the beginning, a detail that allows planes to land at a lower speed than they took off at. Given that landings are naturally more challenging than takeoffs, reducing the landing speed is always helpful. But a nuclear powered aircraft can weigh virtually exactly the same after a two-day mission as it did at the beginning. The plane lands at its gross weight, minus whatever payload it might have dropped. This makes landings difficult in many ways… not only on the pilot, but also the landing gear and the rest of the structure. In April of 1949 a conference held at Oak Ridge National Laboratory in Tennessee included representatives from the Air Force, the Atomic Energy Commission, the Navy and several industry contractors. The result was the birth of the Aircraft Nuclear Propulsion (ANP) programme, a turn from theoretical studies towards a more engineering development effort. The design of aircraft and engines began in earnest.
Lockheed L-195-A-13
Dating from 1949, the L-195 series was the earliest known serious design effort from Lockheed to develop a nuclear powered bomber. Unfortunately very little technical information is available on this and related designs apart from a few drawings. It is unknown if this was work contracted under the NEPA programme, though it seems likely. The L-195-A-13 design featured a nuclear reactor mounted well aft, nearly in the tail. This was counterbalanced by an extremely long forward fuselage with a cramped cockpit located near the nose; 5
Lockheed L-195-A-13
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undoubtedly there would have been a massive lead and plastic radiation shield behind and around the cockpit. The turbojets, of uncertain number, were located in an annular cluster wrapped around the fuselage, just ahead of the straight wing. The payload bay was located aft of the engine cluster but ahead of the reactor. This was clearly an ‘indirect’ system, with long tubes leading from the reactor to the engines. As the engines were all clustered together, the piping would at least have been relatively straightforward and located securely within the central fuselage. Performance, payload and nuclear reactor data are all absent. It was almost certainly meant to be supersonic given the sleek lines and, importantly, the very thin F-104-like wing. Supersonic speeds may have been achieved only with chemical fuel afterburning. Total length was 225ft.
Lockheed NEPA A-7
From January to March of 1950, a small Lockheed Aircraft Corporation contract (a total of 2.1 manmonths… a very minor study) under NEPA resulted in a series of preliminary aircraft designs based on a common core fuselage. A primary feature was described as the 165ft separation distance between the crew cabin and the reactor, providing structural shielding a substantial distance between crew and reactor. The reactor was immediately ahead of a ring of turbojets; this design used eight jet engines. The fairly enormous generic design was just a planned starting point… many wing areas, wing sweeps, engine numbers, gross weights and maximum speeds and altitudes were considered, but solely as a guide for future study. Designs featured sweep from 0° to 60°; this was not a variable geometry design, but a single basic aircraft that could have a number of different wings attached to it. This was to study performance potential with various planforms, gross weights and thrust levels. The unswept wing was, unsurprisingly, restricted to subsonic speeds, and even the most highly swept designs did not greatly exceed the speed of sound. Configuration A-7, shown here, had a 60° wing sweep, and had a maximum airspeed of Mach 1.12 at 35,000ft; its maximum speed at sea level, though, was a creditable Mach 0.97. Curiously, configuration A-9 was able to achieve Mach 1.5 at sea level with 45° wing sweep… or above Mach 1.5 at sea level with a wing sweep of only 15°. Given the minimal study, these numbers are likely highly tentative and were meant to be used to help guide future studies.
Fairchild NEPA N-3
Fairchild was the first company to be contracted to work on atomic propelled aircraft, and produced several designs for supersonic atomic-powered bombers.
Unfortunately, the available information on these early designs presents configurations that are best described as ‘crude’. It may well be that these designs truly were only roughly designed, or it may be that detailed and well considered designs were reproduced with reduced fidelity. A brochure produced by Fairchild in 1951 described a range of nuclear powered bombers; most were subsonic, but two were supersonic. The N-3 design was a rotund vehicle with a centrally located reactor surrounded by an annular ring of six turbojets, each generating 11,900lb of thrust. In the brochure the engine is described as an ‘open’ or ‘air’ cycle, otherwise known as a Direct Cycle type where the air that passed through the compressor then goes directly through the reactor, then out through the turbines. The reactor wall temperature was 2,500°F, while the turbine air inlet temperature was 1,900°F. The overall configuration, apart from the annular engine cluster, was recognizably ‘1950s’, with midmounted thin (3%) tapering unswept wings. The canopy was small but raised, providing a fair bit of visibility for the pilot (and only the pilot). The vertical fin was unusually ‘curvy’. No indication is given in the available art or diagrams about the arrangement of control surfaces.
Fairchild NEPA N-4
The propulsion system for the N-4 used a ‘compound liquid metal cycle’. This variation of the Indirect Cycle used two loops of liquid metal (lithium in both cases)… one passed through the reactor and into a heat exchanger; another loop of liquid metal passed through the heat exchanger and then into the turbojets, replacing the combustors. The reactor had a wall temperature of 1,840°F (doubtless due to the more efficient liquid lithium heat exchange medium) and a turbine air inlet temperature of 1,500°F. The annular ring included ten turbojets, each producing 6,580lb of thrust, around the reactor. The N-4 was in many ways a lower performance system, but where the N-3 cruised at Mach 1.5 at 35,000ft, the N-4 did so at 45,000ft. The layout was similar to that of the N-3, but stretched in various ways. The wing was similar, but set low; the vertical tail was larger and straighter, less generally cartoonish in appearance. The cockpit canopy was smoothly faired into the nose contours, providing a poorer view, but also lower drag and likely better radiation shielding. Like the N-3, though, the general impression is of a very preliminary concept.
North American Aviation Sodium Vapour Compressor Jet
In 1952 North American Aviation issued a report describing an unusual type of nuclear turbojet applied to a supersonic bomber, work that had been 7
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done in 1951 under contract to the Atomic Energy Commission. North American suggested a “sodium vapour compressor jet” as a means of providing the thrust needed for a cruise speed of Mach 1.5. Sodium metal would not be simply melted but boiled to vapour (at 271lb per second). Sodium would, however, not be the cooling fluid for the reactor; instead, tin would cycle through the reactor to extract heat; a heat exchanger would pass that energy to a loop of liquid sodium. This would require increasing the wall temperature of the reactor from the then-achievable 1,500°F to at least 1,800°F… with the possibility that a reactor temperature of 3,000°F might be necessary (considered attainable with a graphite reactor in a nonoxidizing environment). This uncertainty was due to the technology being in its infancy at the time. Unlike most nuclear turbojets, the thermal energy from the reactor was not used to replace the chemical combustors of normal turbojets. Instead, the “compressor jets” were composed of compressor stages attached directly to the turbine stages. The superheated pressurized metallic gas would be used to directly drive the turbines; the air flowing through the compressor would, unlike in a turbojet, not pass through the turbine section. The sodium would be a lower pressure mix of vapour and liquid after passing through the turbines; it would be cooled further – and pressure dropped – by
running it through a heat exchanger behind the turbojet exhausts. The heat exchanger would superheat the air running downstream of the engines and would serve as a nuclear afterburner. The cooled, lower-pressure sodium would be collected and pumped back up to a higher pressure and re-run through the reactor. The loop would continue indefinitely. The aircraft carried a single reactor and five compressor-jet engines. A row of three engines sideby-side were topped by two engines side-by-side, fed from a common plenum that was itself fed from two fuselage-side inlets, and exhausting through a common duct through the tail. The aircraft was of a fairly conventional (for the time) configuration, with thin swept wings and a conventional tail. The forward fuselage was pointed and featureless; a canopy appears to be visible in the available diagram and artwork, but, unusually, the canopy is on the underside of the nose. This indicates that vision for landing was considered paramount. The crew (a rather large number, seven) were housed within a single shielded compartment. The payload was listed as being 20,000lb, but not described further.
NACA Manned Nuclear Designs
The National Advisory Council on Aeronautics spent much of the 1950s looking at nuclear powered flight
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from a more theoretical standpoint. The NACA’s job was not to do detailed engineering designs of aircraft but to do the basic science; what they learned would then be used by the American aviation industry to produce actual products. But the NACA did from time to time produce aircraft designs; supersonic nuclear powered bombers were no exception to this rule. Two such concepts have come to light. From February to September 1952, staff at the NACA Lewis Laboratory studied a manned supersonic aircraft powered by a direct cycle nuclear turbojet engine. The configuration was geometrically simple, being much like a stretched and scaled-up Convair XP-92: a cylindrical fuselage with a very long conical nose, backed by an annular inlet for the engine and a long tapering rear fuselage terminating in a circular exhaust. The wings and vertical tail were simple deltas, 4% thick double-wedge sections. There was no elegance to the design, but the form of the aircraft was not the point of the exercise. Instead, the goal was to demonstrate the possibility of supersonic flight (Mach 1.5 at 35,000ft) with the engine envisioned. The reactor was located in the centre of the fuselage, surrounded by six turbojets. A water shield surrounded the reactor and a lead shadow-shield was placed ahead of it to protect the crew. The compressors at the front of the engines would dump high pressure air into a common plenum and then pass through the water shield and into the reactor; after being heated, the air would leave the reactor into another common plenum at the rear, then pass through the six individual turbine sections, then out the exhaust nozzle. The compressors and turbines would be lined up and the drive shafts would straddle the reactor, passing through the water shield. A range of vehicle and reactor sizes were studied, all based on the same performance requirements. The design shown here is the ‘Case IIA’ configuration, a conservative concept based on ceramic fuel elements with a core temperature of 2660° Rankine and a turbine inlet temperature of 2,000° Rankine. The reactor would be 8.5ft in diameter, 3.14ft long and would produce 504,000 Btu/sec of heat. There was a very sizable cockpit transparency, but that was just the aerodynamic fairing. Behind the very large panes of relatively thin glass or plastic were the much smaller, much thicker windows of the lead and plastic shielded crew compartment. No indication is given of the payload or location of the payload bay, though it would be reasonable to assume it would have been located in the cylindrical section of the fuselage ahead of the inlets. Even before the 1950s, nuclear ramjets were envisioned under project NEPA. While the bulk of the work done for NEPA and its successor ANP was 12
aimed at nuclear powered turboprops and turbojets, the nuclear ramjet was nonetheless understood to have some potential value. The ramjet’s advantage – high speed – did not compare well to its disadvantages – poor subsonic performance, and virtually no lowspeed performance. Consequently few nuclear ramjet configurations were proposed for manned aircraft. But ‘few’ is not the same as ‘none’. A NACA concept from 1957 used two General Electric AC-210 nuclear ramjets located side by side at the rear of the fuselage. This design was done to even less engineering fidelity than the earlier NACA concept if the sole document known on the subject is accurate; only a simplistic top view is known. Consequently, the side and front views reproduced here are fairly speculative. At the request of the Air Force a preliminary design was performed at the NACA Lewis Flight Propulsion Laboratory for an aircraft capable of cruising at Mach 4.25 with a crew of one while carrying a 10,000lb payload. The NACA report does not describe the aircraft as a bomber, but several details point to that being the role. This design put the cockpit roughly in the middle of the fuselage, rather that at the forward end. This drove the need for a massive shield surrounding the cockpit, in this case made of lead and water. The pilot had no direct vision to the outside world. Ahead of the cockpit was a cylindrical volume for ‘instruments’, and ahead of that was another cylindrical volume for ‘payload’. The payload is described solely as weighing 10,000lb… a common generic weight for a single nuclear bomb. In this case it seems the bomb would be carried in a vertical orientation. The nuclear ramjets were optimized for cruise, and would have struggled to produce meaningful thrust below Mach 2.5. Consequently, the aircraft would have required some form of booster; that was left undefined, but likely would have been a sizable verticallylaunched rocket system.
Lockheed CL-285-815
The CL-285-815 was one of a series of designs for nuclear powered supersonic bombers produced by Lockheed in 1954. While details on this and other CL-285 designs are extremely lean, what is clear is that this was a somewhat confusing design. It was meant to attain Mach 2.85; this indicates that the long straight outer wing panels were to be jettisoned. This arrangement is quite similar to that of the ‘three ship formations’ produced by Boeing and North American in 1955 in response to the requirements of WS 110A (see US Supersonic Bomber Projects Volume 1). While the extra wing area would allow the aircraft to loiter or cruise at lower power (and thus radiation) levels,
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